• Acta Optica Sinica
  • Vol. 45, Issue 5, 0530002 (2025)
Lang Yu1, Xiangjun Li1,2,*, and Dexian Yan1,2
Author Affiliations
  • 1College of Information Engineering, China Jiliang University, Hangzhou 310018, Zhejiang , China
  • 2Center for THz Research, China Jiliang University, Hangzhou 310018, Zhejiang , China
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    DOI: 10.3788/AOS241860 Cite this Article Set citation alerts
    Lang Yu, Xiangjun Li, Dexian Yan. Enhanced Terahertz Absorption Spectrum Based on One‐Dimensional Photonic Crystal Defect Modes with Metal‐Dielectric Periodic Structures[J]. Acta Optica Sinica, 2025, 45(5): 0530002 Copy Citation Text show less
    Enhanced terahertz absorption spectrum structure based on one-dimensional photonic crystal defect modes of metal-dielectric periodic structures, and its influence on transmission spectrum. (a) Schematic diagram of structure; (b) transmission spectra of one-dimensional photonic crystal structure and defective one-dimensional photonic crystal structure; (c) transmission spectra of defective one-dimensional photonic crystal structure changing with tilt angle
    Fig. 1. Enhanced terahertz absorption spectrum structure based on one-dimensional photonic crystal defect modes of metal-dielectric periodic structures, and its influence on transmission spectrum. (a) Schematic diagram of structure; (b) transmission spectra of one-dimensional photonic crystal structure and defective one-dimensional photonic crystal structure; (c) transmission spectra of defective one-dimensional photonic crystal structure changing with tilt angle
    Influence of designed structure on spectra of 1.0 μm α-lactose film. (a) Transmission and reflection spectra without α-lactose; (b) transmission and reflection spectra with 1.0 μm α-lactose film; (c) real and imaginary parts of dielectric constant of lactose at 0.48‒0.58 THz; (d) absorption spectra
    Fig. 2. Influence of designed structure on spectra of 1.0 μm α-lactose film. (a) Transmission and reflection spectra without α-lactose; (b) transmission and reflection spectra with 1.0 μm α-lactose film; (c) real and imaginary parts of dielectric constant of lactose at 0.48‒0.58 THz; (d) absorption spectra
    Influences of metal structures and N value on enhanced absorption spectra. (a)‒(d) Influences of metal structures on enhanced absorption spectra; (e)‒(f) influences of metal structures on maximum electric field intensity
    Fig. 3. Influences of metal structures and N value on enhanced absorption spectra. (a)‒(d) Influences of metal structures on enhanced absorption spectra; (e)‒(f) influences of metal structures on maximum electric field intensity
    Electric field distributions at resonant peaks with or without metal structures. (a) Without metal structures; (b) with metal structures
    Fig. 4. Electric field distributions at resonant peaks with or without metal structures. (a) Without metal structures; (b) with metal structures
    Electric field intensity of designed structure. (a) Electric field distributions without α-lactose at different resonance peaks; (b) electric field distributions with α-lactose at different resonance peaks; (c) maximum electric field intensities corresponding to different heights h without α-lactose; (d) comparison of resonance peak intensities
    Fig. 5. Electric field intensity of designed structure. (a) Electric field distributions without α-lactose at different resonance peaks; (b) electric field distributions with α-lactose at different resonance peaks; (c) maximum electric field intensities corresponding to different heights h without α-lactose; (d) comparison of resonance peak intensities
    Influences of N on enhanced absorption spectra. (a)‒(e) N=3‒7; (f) comparisons of results of enhanced absorption spectra with different N from (a)‒(e)
    Fig. 6. Influences of N on enhanced absorption spectra. (a)(e) N=37; (f) comparisons of results of enhanced absorption spectra with different N from (a)(e)
    Influences of α-lactose film thickness t on enhanced absorption spectra. (a)‒(e) t=0.2‒1.0 μm; (f) comparisons of results of enhanced absorption spectra with different t from (a)‒(e)
    Fig. 7. Influences of α-lactose film thickness t on enhanced absorption spectra. (a)‒(e) t=0.2‒1.0 μm; (f) comparisons of results of enhanced absorption spectra with different t from (a)‒(e)
    Influences of dielectric height h on enhanced absorption spectra. (a)‒(e) h=10‒70 μm; (f) comparisons of results of enhanced absorption spectra with different h from (a)‒(e)
    Fig. 8. Influences of dielectric height h on enhanced absorption spectra. (a)‒(e) h=10‒70 μm; (f) comparisons of results of enhanced absorption spectra with different h from (a)‒(e)
    Influences of metal width w on enhanced absorption spectra. (a)‒(e) w=1‒5 μm; (f) comparisons of results of enhanced absorption spectra with different w from (a)‒(e)
    Fig. 9. Influences of metal width w on enhanced absorption spectra. (a)‒(e) w=1‒5 μm; (f) comparisons of results of enhanced absorption spectra with different w from (a)‒(e)
    ReferenceCell structureAnalyte (thickness)Multiplexing modeWorking bandEnhancement factor
    28Dielectric metagratinghBN(0.34 nm)Angle

    Mid

    infrared

    ~30
    14Dielectric metagratingα-lactose(1.0 µm)AngleTHz~20
    21One-dimensional photonic crystal defect modes in high-resistance silicon

    α-lactose

    (0.2 µm)

    Air gapTHz~55
    25Teflon one-dimensional photonic crystal defect modeα-lactose(1.0 µm)Air gapTHz~41

    This

    work

    One-dimensional photonic crystal defect modes in metal-dielectric periodic structures

    α-lactose

    (0.2 µm)

    Air gapTHz~101.2
    This workDielectric one-dimensional photonic crystal defect modeα-lactose(0.2 µm)Air gapTHz~76.2
    Table 1. Comparison of operational performance among similar structures and designed structures
    Lang Yu, Xiangjun Li, Dexian Yan. Enhanced Terahertz Absorption Spectrum Based on One‐Dimensional Photonic Crystal Defect Modes with Metal‐Dielectric Periodic Structures[J]. Acta Optica Sinica, 2025, 45(5): 0530002
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